Assignment 1 with Solution | Applied Thermodynamics | M E 320, Assignments of Thermodynamics

Material Type: Assignment; Professor: Deinert; Class: APPLIED THERMODYNAMICS; Subject: Mechanical Engineering; University: University of Texas - Austin; Term: Fall 2009;

Typology: Assignments

Pre 2010

Uploaded on 11/03/2009

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1.4) An object has a mass of 10 lb. Determine its weight, in lbf, at a location where the acceleration of
gravity is 31.0 ft/s2.
๐‘€๐‘Ž๐‘ ๐‘  =10 ๐‘™๐‘ ๐‘ฅ 0.4536 ๐‘˜๐‘”
1 ๐‘™๐‘ = 4.536 ๐‘˜๐‘”
๐‘” = 31.0 ๐‘“๐‘ก
๐‘ 2 ๐‘ฅ 1 ๐‘š
3.2808 ๐‘“๐‘ก = 9.5 ๐‘š/๐‘ 2
๐‘ค๐‘’๐‘–๐‘”๐‘•๐‘ก = ๐น๐‘”=๐‘š๐‘Ž =๐‘š๐‘” = 4.536 ๐‘˜๐‘” (9.5 ๐‘š
๐‘ 2)
weight = 43.092 N โ‰ˆ43.1 N
๐‘ค๐‘’๐‘–๐‘”๐‘•๐‘ก = 43.1๐‘ ๐‘ฅ 0.22481 ๐‘™๐‘๐‘“
1 ๐‘= 9.67 ๐‘™๐‘๐‘“ ANS
1.31) A gas contained within a piston-cylinder assembly undergoes three processes in series:
Process 1-2: Compression with pV =constant from p1 = 1 bar, V1 = 1.0 m3 to V2 = 0.2 m3
Process 2-3: Constant-=pressure expansion to V3 = 1.0 m3
Process 3-1: Constant volume
Sketch the processes in series on a p-V diagram labeled with pressure and volume values at each
numbered state.
First determine the pressures and volumes at each of the states (only P2 unknown):
P2 = ?
P1V1 = P2V2 (Process 1-2 has pV = constant)
๐‘ƒ2=๐‘ƒ1๐‘‰1
๐‘‰2
= 1 ๐‘๐‘Ž๐‘Ÿ (1.0 ๐‘š3)
(0.2 ๐‘š3) = 5 ๐‘๐‘Ž๐‘Ÿ๐‘ 
State
Pressure (bars)
Volume (m3)
1
1
1
2
5
0.2
3
5
1
pf3
pf4
pf5

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1.4) An object has a mass of 10 lb. Determine its weight, in lbf, at a location where the acceleration of gravity is 31.0 ft/s^2.

1 ๐‘™๐‘ = 4.536^ ๐‘˜๐‘”

๐‘ ^2 ๐‘ฅ^

3.2808 ๐‘“๐‘ก = 9.5^ ๐‘š/๐‘ 

2

๐‘ ^2 )

weight = 43.092 N โ‰ˆ43.1 N

๐‘ค๐‘’๐‘–๐‘”๐‘•๐‘ก = 43. 1 ๐‘ ๐‘ฅ 0.^224811 ๐‘ ๐‘™๐‘๐‘“= 9. 67 ๐‘™๐‘๐‘“ ANS

1.31) A gas contained within a piston-cylinder assembly undergoes three processes in series:

Process 1-2 : Compression with pV =constant from p 1 = 1 bar, V 1 = 1.0 m^3 to V 2 = 0.2 m^3

Process 2-3 : Constant-=pressure expansion to V 3 = 1.0 m^3

Process 3-1 : Constant volume

Sketch the processes in series on a p-V diagram labeled with pressure and volume values at each numbered state.

First determine the pressures and volumes at each of the states (only P 2 unknown):

P 2 =?

P 1 V 1 = P 2 V 2 (Process 1-2 has pV = constant)

๐‘‰ 2 =^

1 ๐‘๐‘Ž๐‘Ÿ (1.0 ๐‘š^3 )

(0.2 ๐‘š^3 ) = 5^ ๐‘๐‘Ž๐‘Ÿ๐‘ 

State Pressure (bars) Volume (m^3 ) 1 1 1 2 5 0. 3 5 1

Sketch the process and label the states and their pV values (labeled as (p,V)):

1.34) The absolute pressure inside a tank is 0.4 bars, and the surroundings atmospheric pressure is 98 kPa. What reading would a Bourdon gage mounted in the tank wall give, in kPa? Is this a gage or vacuum reading?

First convert bars to kPa:

1 ๐‘ฅ 105 ๐‘/๐‘š^2

1 ๐‘/๐‘š^2

A Bourdon gage measures the difference between the absolute internal pressure and the absolute outside pressure. In this case the tank pressure and the atmospheric pressure. Since the atmospheric pressure is greater than the tank pressure, the measured pressure will be a vacuum pressure:

2.1) A baseball has a mass of 0.3 lb. What is the kinetic energy relative to home plate of a 94 mile per hour fastball, in Btu?

2

Converting from English to SI units:

2.2046 ๐‘™๐‘ = 0.136^ ๐‘˜๐‘”

1 ๐‘š๐‘๐‘• = 151.27^ ๐‘˜๐‘š/๐‘•

Solving for the kinetic energy:

๐‘˜๐‘š^2

๐‘•^2

(1๐‘ฅ 103 ๐‘š)^2

(1 ๐‘˜๐‘š)^2

(1 ๐‘•)^2

(60 ๐‘š๐‘–๐‘›)^2

(1 ๐‘š๐‘–๐‘›)^2

(60 ๐‘ )^2

๐‘š^2

๐‘ ^2

๐‘š^2

๐‘ ^2 ๐‘ฅ^

๐‘˜๐‘” ๐‘š/๐‘ ^2 = 120.83^ ๐‘^ ๐‘š^ ๐‘ฅ^

1 ๐‘ ๐‘š = 120.83^ ๐ฝ

Converting final answer into Btu yields:

1000 ๐ฝ ๐‘ฅ^

1 ๐‘˜๐ฝ =^0.^1145 ๐ต๐‘ก๐‘ข

๐พ๐ธ = 0.1145 ๐ต๐‘ก๐‘ข ANS

2.20) The drag force, Fd, imposed by the surrounding air on a vehicle moving with velocity V is given by:

F (^) d = Cd A^12 ฯV^2

where Cd is a constant called the drag coefficient, A is the projected frontal area of the vehicle, and ฯ is the air density. Determine the power, in kW, required to overcome aerodynamic drag for a truck moving at 110 km/h, if Cd = 0.65, A = 10m^2 , and ฯ = 1.1 kg/m^3.

Solving for the draq force Fd yields:

F (^) d = Cd A^12 ฯV^2

๐น๐‘‘ = 0.65 10 ๐‘š^2 0.5 1.

๐‘š^3 (^

2

๐‘š^2 ๐‘˜๐‘š^2

๐‘š^3 ๐‘•^2 = 4.326๐‘ฅ^10

2 ๐‘š ๐‘•^2

๐น๐‘‘ = 4.326๐‘ฅ 104 ๐‘˜๐‘”

๐‘˜๐‘š^2

๐‘š ๐‘•^2

(1000 ๐‘š)^2

(1๐‘˜๐‘š)^2

(1 ๐‘•)^2

(3600๐‘ )^2

๐‘˜๐‘” ๐‘š/๐‘ ^2

Solving for the power:

๐‘Š = ๐น โˆ™ ๐‘‰ = ๐น ๐‘‰ cos ๐œƒ

Since the drag force acts directly opposite the velocity, ฮธ = 180

๐‘Š๐‘‘ = 3.338๐‘ฅ 103 ๐‘

cos 180 = 3.338๐‘ฅ 103 110

๐‘• ๐‘ฅ^

1 ๐‘˜๐‘š ๐‘ฅ^

3600 ๐‘  ๐‘ฅ^

1 ๐‘๐‘š ๐‘ฅ^

1 ๐ฝ/๐‘  =^ โˆ’1.02๐‘ฅ^10

The power required to overcome this aerodynamic drag force is the opposite of the value calculated above, therefore:

๐‘Š = โˆ’๐‘Š๐‘‘ = +1.02๐‘ฅ 105 ๐‘Š ๐‘ฅ

๐‘Š = 102 ๐‘˜๐‘Š ANS